Deformation of the proton emitter 113Cs from electromagnetic transition and proton-emission rates

D. Hodge; D. M. Cullen; M. J. Taylor; B. S. Nara Singh; L. S. Ferreira; E. Maglione; J. F. Smith; C. Scholey; P. Rahkila; T. Grahn; Th. Braunroth; H. Badran; L. Capponi; A. Girka; P.T. Greenlees; R. Julin; J. Konki; M. Mallaburn; O. Nefodov; G. G. O'Neill; J. Pakarinen; Phillipos Papadakis; J. Partanen; P. Ruotsalainen; M. Sandzelius; J. Sarén; M. Smolen; J. Sorri; S. Stolze; J. Uusitalo

doi:10.1103/PhysRevC.94.034321

Deformation of the proton emitter ¹¹³Cs from electromagnetic transition and proton-emission rates

D. Hodge
, D. M. Cullen
, M. J. Taylor
, B. S. Nara Singh
, L. S. Ferreira
, E. Maglione
, J. F. Smith
, C. Scholey
, P. Rahkila
, T. Grahn
, Th. Braunroth
, H. Badran
, L. Capponi
, A. Girka
, P.T. Greenlees
, R. Julin
, J. Konki
, M. Mallaburn
, O. Nefodov
, G. G. O'Neill

J. Pakarinen, Phillipos Papadakis, J. Partanen, P. Ruotsalainen, M. Sandzelius, J. Sarén, M. Smolen, J. Sorri, S. Stolze, J. Uusitalo

School of Computing, Engineering and Physical Sciences

Research output: Contribution to journal › Article › peer-review

5 Citations (Scopus)

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Abstract

The lifetime of the (11/2⁺) state in the band above the proton-emitting (3/2⁺) state in ¹¹³Cs has been measured to be τ=24(6) ps from a recoil-decay-tagged differential-plunger experiment. The measured lifetime was used to deduce the deformation of the states using wave functions from a nonadiabatic quasiparticle model to independently calculate both proton-emission and electromagnetic γ-ray transition rates as a function of deformation. The only quadrupole deformation, which was able to reproduce the experimental excitation energies of the states, the electromagnetic decay rate of the (11/2⁺) state and the proton-emission rate of the (3/2⁺) state, was found to be β₂=0.22(6). This deformation is in agreement with the earlier proton emission studies which concluded that ¹¹³Cs was best described as a deformed proton emitter, however, it is now more firmly supported by the present measurement of the electromagnetic transition rate.

Original language	English
Article number	034321
Number of pages	8
Journal	Physical Review C
Volume	94
Early online date	21 Sept 2016
DOIs	https://doi.org/10.1103/PhysRevC.94.034321
Publication status	Published - 21 Sept 2016

Keywords

collective models
electromagnetic transitions
lifetimes and widths
nuclear structure and decays
proton emission
spectroscopic factors andelectromagnetic moments

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10.1103/PhysRevC.94.034321Licence: CC BY

2016 09 21 Hodge et al DeformationFinal published version, 475 KBLicence: CC BY

Sreenivasa Bondili
- School of Computing, Engineering and Physical Sciences - Lecturer
Person: Academic

Cite this

Hodge, D., Cullen, D. M., Taylor, M. J., Nara Singh, B. S., Ferreira, L. S., Maglione, E., Smith, J. F., Scholey, C., Rahkila, P., Grahn, T., Braunroth, T., Badran, H., Capponi, L., Girka, A., Greenlees, P. T., Julin, R., Konki, J., Mallaburn, M., Nefodov, O., ... Uusitalo, J. (2016). Deformation of the proton emitter ¹¹³Cs from electromagnetic transition and proton-emission rates. Physical Review C, 94, Article 034321. https://doi.org/10.1103/PhysRevC.94.034321

@article{9866d8ea3b2046369356ce193c929317,

title = "Deformation of the proton emitter 113Cs from electromagnetic transition and proton-emission rates",

abstract = "The lifetime of the (11/2+) state in the band above the proton-emitting (3/2+) state in 113Cs has been measured to be τ=24(6) ps from a recoil-decay-tagged differential-plunger experiment. The measured lifetime was used to deduce the deformation of the states using wave functions from a nonadiabatic quasiparticle model to independently calculate both proton-emission and electromagnetic γ-ray transition rates as a function of deformation. The only quadrupole deformation, which was able to reproduce the experimental excitation energies of the states, the electromagnetic decay rate of the (11/2+) state and the proton-emission rate of the (3/2+) state, was found to be β2=0.22(6). This deformation is in agreement with the earlier proton emission studies which concluded that 113Cs was best described as a deformed proton emitter, however, it is now more firmly supported by the present measurement of the electromagnetic transition rate.",

keywords = "collective models, electromagnetic transitions, lifetimes and widths, nuclear structure and decays, proton emission, spectroscopic factors andelectromagnetic moments",

author = "D. Hodge and Cullen, \{D. M.\} and Taylor, \{M. J.\} and \{Nara Singh\}, \{B. S.\} and Ferreira, \{L. S.\} and E. Maglione and Smith, \{J. F.\} and C. Scholey and P. Rahkila and T. Grahn and Th. Braunroth and H. Badran and L. Capponi and A. Girka and P.T. Greenlees and R. Julin and J. Konki and M. Mallaburn and O. Nefodov and O'Neill, \{G. G.\} and J. Pakarinen and Phillipos Papadakis and J. Partanen and P. Ruotsalainen and M. Sandzelius and J. Sar{\'e}n and M. Smolen and J. Sorri and S. Stolze and J. Uusitalo",

year = "2016",

month = sep,

day = "21",

doi = "10.1103/PhysRevC.94.034321",

language = "English",

volume = "94",

journal = "Physical Review C",

issn = "2469-9985",

publisher = "American Physical Society",

}

Hodge, D, Cullen, DM, Taylor, MJ, Nara Singh, BS, Ferreira, LS, Maglione, E, Smith, JF, Scholey, C, Rahkila, P, Grahn, T, Braunroth, T, Badran, H, Capponi, L, Girka, A, Greenlees, PT, Julin, R, Konki, J, Mallaburn, M, Nefodov, O, O'Neill, GG, Pakarinen, J, Papadakis, P, Partanen, J, Ruotsalainen, P, Sandzelius, M, Sarén, J, Smolen, M, Sorri, J, Stolze, S & Uusitalo, J 2016, 'Deformation of the proton emitter ¹¹³Cs from electromagnetic transition and proton-emission rates', Physical Review C, vol. 94, 034321. https://doi.org/10.1103/PhysRevC.94.034321

TY - JOUR

T1 - Deformation of the proton emitter 113Cs from electromagnetic transition and proton-emission rates

AU - Hodge, D.

AU - Cullen, D. M.

AU - Taylor, M. J.

AU - Nara Singh, B. S.

AU - Ferreira, L. S.

AU - Maglione, E.

AU - Smith, J. F.

AU - Scholey, C.

AU - Rahkila, P.

AU - Grahn, T.

AU - Braunroth, Th.

AU - Badran, H.

AU - Capponi, L.

AU - Girka, A.

AU - Greenlees, P.T.

AU - Julin, R.

AU - Konki, J.

AU - Mallaburn, M.

AU - Nefodov, O.

AU - O'Neill, G. G.

AU - Pakarinen, J.

AU - Papadakis, Phillipos

AU - Partanen, J.

AU - Ruotsalainen, P.

AU - Sandzelius, M.

AU - Sarén, J.

AU - Smolen, M.

AU - Sorri, J.

AU - Stolze, S.

AU - Uusitalo, J.

PY - 2016/9/21

Y1 - 2016/9/21

N2 - The lifetime of the (11/2+) state in the band above the proton-emitting (3/2+) state in 113Cs has been measured to be τ=24(6) ps from a recoil-decay-tagged differential-plunger experiment. The measured lifetime was used to deduce the deformation of the states using wave functions from a nonadiabatic quasiparticle model to independently calculate both proton-emission and electromagnetic γ-ray transition rates as a function of deformation. The only quadrupole deformation, which was able to reproduce the experimental excitation energies of the states, the electromagnetic decay rate of the (11/2+) state and the proton-emission rate of the (3/2+) state, was found to be β2=0.22(6). This deformation is in agreement with the earlier proton emission studies which concluded that 113Cs was best described as a deformed proton emitter, however, it is now more firmly supported by the present measurement of the electromagnetic transition rate.

AB - The lifetime of the (11/2+) state in the band above the proton-emitting (3/2+) state in 113Cs has been measured to be τ=24(6) ps from a recoil-decay-tagged differential-plunger experiment. The measured lifetime was used to deduce the deformation of the states using wave functions from a nonadiabatic quasiparticle model to independently calculate both proton-emission and electromagnetic γ-ray transition rates as a function of deformation. The only quadrupole deformation, which was able to reproduce the experimental excitation energies of the states, the electromagnetic decay rate of the (11/2+) state and the proton-emission rate of the (3/2+) state, was found to be β2=0.22(6). This deformation is in agreement with the earlier proton emission studies which concluded that 113Cs was best described as a deformed proton emitter, however, it is now more firmly supported by the present measurement of the electromagnetic transition rate.

KW - collective models

KW - electromagnetic transitions

KW - lifetimes and widths

KW - nuclear structure and decays

KW - proton emission

KW - spectroscopic factors andelectromagnetic moments

U2 - 10.1103/PhysRevC.94.034321

DO - 10.1103/PhysRevC.94.034321

M3 - Article

SN - 2469-9985

VL - 94

JO - Physical Review C

JF - Physical Review C

M1 - 034321

ER -

Deformation of the proton emitter 113Cs from electromagnetic transition and proton-emission rates

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Keywords

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Sreenivasa Bondili

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Deformation of the proton emitter ¹¹³Cs from electromagnetic transition and proton-emission rates